EP3234680A1

EP3234680A1 - Scanning microscope

Info

Publication number: EP3234680A1
Application number: EP15817826.9A
Authority: EP
Inventors: Jonas FÖLLING
Original assignee: Leica Microsystems CMS GmbH
Current assignee: Leica Microsystems CMS GmbH
Priority date: 2014-12-19
Filing date: 2015-12-21
Publication date: 2017-10-25
Also published as: US20170351071A1; LU92620B1; JP2018501515A; WO2016097399A1; US10663707B2

Abstract

The invention relates to a scanning microscope (100), comprising an objective (112) which focuses an illumination beam (102) at a specimen (115), a scanning element (104), which is arranged upstream of the objective (112) and which can be adjusted in order to deflect the illumination beam (102) in a time-varying manner in order to guide the focused illumination beam (102) across the specimen (115) in a scanning motion, and an image sensor (122), onto which the objective (112) focuses a detection beam (114) originating at the specimen (115) illuminated with the focused illumination beam (102). The image sensor (122) has a plurality of sensor elements (124) which can be individually read out by a controller (126) and across which the detection beam (114) is guided in a motion corresponding to the scanning motion of the focused illumination beam (102). A dispersive element (120) of predetermined dispersion effect is provided, which spatially separates different spectral components of the detection beam (114) from each other on the image sensor (122). The controller (126) senses the time-varying adjustment of the scanning element (104), assigns the spectral components of the detection beam (114) to the sensor elements (124) of the image sensor (122) in accordance with said adjustment while taking into account the predetermined dispersion effect of the dispersive element (120), and reads out the sensor elements (124) assigned to the respective spectral components.

Description

scanning microscope

The invention relates to a scanning microscope with a lens that focuses an illumination beam on an object, a lens element upstream grid element, which is adjustable for time-varying deflection of the illumination beam to guide the focused illumination beam in a raster motion over the object, and a

Image sensor, on which the lens possibly in connection with further optics one

Detection beam images or focused, which of the focused with the

Illuminated beam illuminated object emanates, wherein the image sensor has a plurality of individually readable by a control sensor elements over which the detection beam is guided in a movement corresponding to the raster movement of the focused illumination beam.

In scanning microscopy, at least one illumination beam is focused onto a sample by means of an objective. In order to guide the illumination beam in a raster or scanning movement over the sample, the objective is preceded by a raster element (such as, for example, one or more movable mirrors, an AOD, ie an Acousto Optical Deflector or the like), which deflects the illumination beam in such a way that that this on the sample the desired

Raster motion performs. Usually, the grid element comprises one or more mirrors whose tilting movement is converted by the optical imaging into a lateral movement of the light spot generated on the sample by the illumination beam. The focused illumination beam thus scans the sample point by point. The detection light emanating from the sample is then detected for each halftone dot. Finally, the detection signal thus detected is assembled into an image in a computing unit.

In the field of scanning microscopy confocal microscopy represents a particularly preferred microscopy method. The basic operation of this

Microscopy method is explained below with reference to Figure 1, in which a designated confocal microscope generally 10 is shown purely schematically.

The confocal microscope 10 has a light source, not shown in FIG

Illuminating beam 12 on a dichroic beam splitter mirror 14 emits. The beam splitter mirror 14 is designed to emit light at the wavelength of the

Illuminating beam 12 lets through. The illumination beam 12 thus passes through the

Beam splitter mirror 14 and falls on a scanning mirror 16. As in Figure 1 by the

Double arrow indicated, the Abtastspiegel 16 is tilted. Due to the tilting movement of the scanning mirror 16, the illumination beam 12 is corresponding to the desired

Distracted raster motion. After reflection on the scanning mirror 16, the illumination beam 12 passes through a

Sensing lens 18 of the focal length f3, a tube lens 20 of the focal length f2 and a lens 22 of the focal length f1. The objective 22 finally focuses the illumination beam 12 onto a sample 24. The tilting movement of the scanning mirror 16 causes the focused image to scan

Illumination beam 12 scans the sample 24 point by point.

A detection beam denoted by 26 in FIG. 1, which starts from a grid point illuminated by the focused illumination beam 12, passes back into the objective 22 and traverses the beam path described above in the opposite direction until it falls onto the beam splitter mirror 14. The latter is designed to reflect light at the wavelength of the detection beam 26. The beam splitter mirror 14 directs the

Detection beam 26 thus on a lens 28, which focuses the detection beam 26 on a confocal aperture plate 30. Through the pinhole 30 is from the

Detection beam 26 filtered out all the light that comes from areas of the sample 24, which originates outside the light spot generated by the illumination beam 12 on the sample 24. The light that passes through the pinhole 30, finally reaches an image sensor 32, which can be read out via a controller 34. The light emanating from the sample 24 can thus be detected for each individual grid point and the detection signal thus generated can be combined to form an image.

An essential feature of the confocal microscope 10 according to FIG. 1 in the present context is that the detection beam 26 emanating from the sample 24 is directed back to the scanning mirror 16, so that the detection beam 26 is influenced in the same way by the scanning mirror 16 As a result, the detection beam 26 is fixedly incident on the image sensor 32, while the illumination beam 12 is detected by the scanning movement of the scanning mirror 16

Raster movement on the sample 24 performs. The detection beam 26 is through this

Feedback on the scanning mirror 16 on the image sensor 32 held stationary as it were. Stationary in this context means that, although the angle of incidence, under which the detection beam 26 falls on the image sensor 32, may vary (in the embodiment of Figure 1, this angle of incidence is stationary), but not the location of light incidence. The principle of holding the detection beam 26 stationary by returning it to the raster element 16 on the image sensor 32 in the above-described sense, is on the

In order to enable such a "descanning", the scanning mirror 16 in the confocal microscope according to FIG. 1 is arranged in a plane 36 which is one of those designated 38 in FIG

Object level represents optically conjugate level. In Figure 1 are also a Intermediate image plane 40 and 42 shown. The intermediate image plane 40 corresponds optically to the plane 36 and is optically conjugate to the object plane 38. The intermediate image plane 42 corresponds optically to the object plane 38 and is optically conjugate to the plane 36.

For many applications in microscopy, it is now important to enable as continuously variable as possible spectral detection. This means that the detection light can be divided into different detection channels as differentiated as possible by wavelength. This is necessary, for example, in order to separate the detection signals originating from different dyes as well as possible from each other. Similarly, different conditions in the sample can be detected by variations in the emission spectrum of a dye. If these variations can be measured by a well-resolved spectral detection, the user can reconstruct the different conditions in the sample.

Such a spectral detection could be realized comparatively easily in a confocal microscope of the type shown in FIG. Reference is made to FIG. 2, which shows the confocal microscope 10 in a modification which permits spectral detection. In the modification according to FIG. 2, a dispersive element 44 is provided in the beam path downstream of the pinhole diaphragm 30, which decomposes the detection beam 26 into its different spectral components and supplies these components to the image sensor 32. The image sensor 32 has a multiplicity of sensor elements which can be individually read out via a controller 34. The various spectral components are illustrated in FIG. 2 by partial beams 26-1 to 26-7. The dispersive element 44 is preceded by a converging lens 46, which bundles the detection beam 26 passing through the perforated diaphragm 30 onto the dispersive element 44.

The modification according to FIG. 2 utilizes the descanning principle used in the confocal microscope 10. Since the detection beam 26 leaves the pinhole 30 as a stationary beam, the various spectral components of the

Detection beam 26 regardless of the currently imaged grid point on the sample 24 by the dispersive element 44 spatially separated from each other in the manner illustrated in Figure 2. For example, via a diaphragm not shown in FIG. 2, exactly the spectral component of interest can then be filtered out of the detection beam 26 and supplied to the image sensor 32.

The situation is different with the so-called "non-descanned" principle, as used in the field of fluorescence microscopy, for example in a multiphoton microscope in the manner illustrated in Figure 3. Figure 3 shows a multiphoton microscope 50 in which a light source, not shown an illumination beam 52 on a tiltable Scanning mirror 54, on which the illumination beam 52 is reflected and then passes through a scanning lens 56 of focal length f3, a tube lens 58 of focal length f2, a dichroic beam splitter mirror 60 and finally a lens 62 of focal length f1 to focus on a sample 64 , A detection beam 66 emanating from the sample 64 illuminated with the focused illumination beam 52 passes back into the objective 62 and is then directed by the dichroic mirror 60 to an image sensor 68 which is coupled to a controller 70. The scanning mirror 54 is located in a plane 72 which is optically conjugate to an image plane 74 in which the sample 64 is located. In Figure 3 further levels 76 and 78 are shown. The level 76 represents a

Intermediate image plane which corresponds optically to the plane 72 and is optically conjugate to the object plane 74. The plane 78 is again an intermediate image plane, the optically

Object level 74 corresponds and is optically conjugate to the level 72.

In contrast to the confocal microscope 10 according to Figures 1 and 2 is in the

Multiphoton microscope 50 of the detection beam 66 through the dichroic

Beam splitter mirror 60 from the leading to the scanning mirror 54 beam path

decoupled and fed directly to the image sensor 70 before it reaches the scanning mirror 54. Accordingly, the detection beam 66 varies both in its angle of incidence and in its incidence on the image sensor 70 when the illumination beam 52 performs its raster motion on the sample 64. The spectral detection according to FIG. 2 is therefore not applicable to the confocal microscope 50 according to FIG. 3, which operates on the non-descanned principle.

The object of the invention is a scanning microscope of the type mentioned so

to further develop that it allows a simple and reliable spectral detection of a falling on an image sensor detection beam.

The invention solves this problem by the scanning microscope with the features of claim 1.

According to the invention, a dispersive element of predetermined dispersion effect, which separates the different spectral components of the detection beam spatially from one another on the image sensor, is provided in the scanning microscope. The controller detects the time-varying adjustment of the raster element, assigns the spatially separated spectral components of the detection beam in consideration of this adjustment, the sensor elements of the image sensor taking into account the

predetermined dispersion effect of the dispersive element and reads out the respective spectral components associated sensor elements to enable the spectrally resolved detection of the detection beam. The solution according to the invention provides for the spatial splitting of the detection beam, which is caused by the spectral separation by means of the dispersive element, to be separated from the spatial movement of the detection beam which is effected by the grid element. For this purpose, the controller detects the present adjustment of the raster element, that is, for example, the tilt angle of a raster element forming the raster element

Scanning mirror assembly, which may be formed of one or more mirrors. The controller also takes into account the previously known dispersion effect of the dispersive element. Based on this information, namely the adjustment of the

Rasterelementes and the dispersion effect of the dispersive element, it is the

Control at any time possible, an exact assignment between the

Sensor elements and the different spectral components of the incident on the image sensor detection beam to make. The manner in which the controller detects the temporally variable adjustment of the raster element is in no way limited. So it is conceivable, for example, that the grid element itself a corresponding

For example, output information directly to the controller via an angle encoder. Likewise, however, a separate sensor can be provided which detects the current adjustment of the grid element and notifies the controller. What the previously known

Concerning dispersion effect of the dispersive element, it may for example be kept in a memory, which is accessed by the controller, to the

To take into account dispersion effects in spectral detection.

Preferably, the dispersive element is disposed in a plane that is optically conjugate to a plane in which the sample is disposed. The plane in which the dispersive

Element is preferably optically equivalent to a plane in which the grid element is arranged. By "optically equivalent" is meant in this context that the two said planes correspond in a manner to each other optically, that the spatial variation of the illumination beam at the location of the grid element is translated into a corresponding spatial variation of the detection beam at the location of the dispersive element the spatial variation of the illumination beam at the location of the raster element in that the illumination beam varies in its angle of incidence, but not in its incident position, this also applies to the detection beam at the location of the dispersive element, ie also the detection beam varies its angle of incidence, but not its If the said optical equivalence is given in this sense, then it is particularly easy to realize the dispersive element suitably, since the incidence position of the detection beam at the dispersive element does not change. Preferably, the raster element guides the illumination beam in a first

Scanning direction over the sample. In this case, for example, the raster element is a single mirror that is rotated about a fixed axis to move the illumination beam preferably straight across the sample in the first scanning direction.

The grid element can additionally illuminate the illumination beam in one of the first

Scanning direction perpendicular second scanning direction over the sample, wherein the movement of the illumination beam in the first scanning direction is faster than in the second scanning direction. In this embodiment, the raster element comprises, for example, two separate scanning mirrors, of which a first mirror, the raster movement in the first scanning direction and the second scanning mirror, the raster movement in the second

Scanned direction causes. However, it may also be provided a single scanning mirror, which is moved in both scanning directions. The one scanning direction in which the illumination beam on the sample moves faster than in the other scanning direction will be referred to simply as a fast scanning direction. Accordingly, the other direction is referred to as a slow scan direction.

Preferably, the dispersion effect of the dispersive element is predetermined such that the spectral components of the detection beam are spatially separated on the image sensor in a direction perpendicular to a direction in which the detection beam is passed over the image sensor when the illumination beam in the first Scanning over the sample is performed. In this embodiment, so is the

Plane in which the detection beam is spectrally split by the dispersive element, parallel to the slow scan direction. As a result of the spectral splitting, the dispersive element generates a "spectral fan" in which the spectral information is encoded in an angle information At the same time the vertex of the scan angle of the raster element is preferably in the plane optically conjugate to the object plane, at the same time the scan angle is superimposed on the angle of the spectral splitting with respect to the slow scan direction, which means that in this embodiment the above-mentioned spectral fan is around that in the slow scan direction At the same time, the spectral fan tilts back and forth with the scan angle relative to the fast scan direction, and the tilting motion in the fast scan direction is perpendicular to the tilt egung in the slow

Scanning direction and is thus decoupled from this. In a particularly preferred embodiment is located between the dispersive element and the image sensor detection optics, which bundles the spectrally split by the dispersive detection beam at each adjustment of the grid element in its entirety on the image sensor. Since it is to be ensured at all times that the detection beam, which performs a movement corresponding to the raster movement of the illumination beam on the image sensor and is also fanned out spatially by the dispersive element, falls in its entirety onto the image sensor, contributes a bundling detection optics of the aforementioned type at, not to let the image sensor too big.

In one embodiment, the detection optics is a lens in whose focal plane the dispersive element is arranged. Such an embodiment can be selected in particular when the image sensor is an area sensor.

The detection optics can also be designed to spectrally split

Detection beam at each adjustment of the locking element along a predetermined line to focus on the image sensor. In this case, a line sensor can be used as the image sensor.

In a particularly preferred embodiment, the detection optics comprises a crossed arrangement of three cylindrical lenses, the middle cylindrical lens of which

has refractive effective cut, which lies in a first plane, while the refractive effective cuts of the other two cylindrical lenses lie in a plane perpendicular to the first plane second plane. With such a cylindrical lens arrangement, the spectrally split detection beam can be particularly easily bundled on a line sensor independently of the currently present adjustment of the raster element.

The controller may be configured to select at least one of the spectral components and to read only those sensor elements which are assigned to this selected spectral component. This allows a particularly efficient spectral detection.

The dispersive element is, for example, a prism or a grating. However, it is not limited to such embodiments. For example, an acousto-optical component such as an AOTF can also be used as a dispersive element.

The solution according to the invention can be used profitably in any type of scanning microscope, but in particular in microscopes that work according to the non-descanned method, ie in which the detection beam is coupled to the image sensor before it reaches the grid element. A particularly preferred application is in multiphoton microscopy, in contrast to the confocal microscopy in favor of an improved signal-to-noise ratio is omitted, due to the detection beam to the grid element and then to pass through a pinhole. So will the

Multiphoton microscopy often used in strongly scattering samples. As a result, the detection light is scattered so much that it no longer seems to originate from the central focus area. Nevertheless, this light should be captured by the image sensor to achieve a better detection signal.

Furthermore, the invention provides a method for scanning microscopic imaging of a sample with the features of claim 15.

The invention will be explained in more detail below with reference to FIGS. Show:

Figure 1 is a schematic representation of a conventional confocal microscope;

FIG. 2 shows an embodiment of the confocal microscope according to FIG. 1 modified for the purpose of spectral detection;

Figure 3 is a schematic representation of a conventional multiphoton microscope;

Figure 4 is a schematic representation of an embodiment of the scanning microscope according to the invention;

Figure 5 is a schematic representation of a usable in the scanning microscope of the invention detection optics in various modifications; and

FIG. 6 shows the detection optics according to FIG. 5 in another sectional view.

Figure 4 shows a purely schematic representation of a scanning microscope 100, which operates on the non-descanned principle. In the scanning microscope 100, a light source, not shown in FIG. 4, emits an illumination beam 102 onto a scanning mirror 104. As indicated by the double arrow in FIG. 4, the scanning mirror 104 can be tilted for variable deflection of the illumination beam 102. In FIG. 4, a first tilted position with a solid line and a second tilted position with a dashed line are shown purely schematically. Accordingly, in the beam path downstream of the

Scanning mirror 104 of the illumination beam 102 for the first tilted position with

solid line and shown for the second tilted position with a dashed line. The reflected on the scanning mirror 104 illumination beam passes successively a scanning lens 106 of the focal length f3, a tube lens 108 of focal length f2, a dichroic beam splitter mirror 1 10 and an objective 1 12 of the focal length f 1, which focuses the illumination beam 102 on a sample 1 15. According to the two Tilting positions of the scanning mirror 104, two grid points are shown in Figure 4, in which the focused by the lens 1 12 illumination beam 102 converges respectively.

A detection beam 1 14, which emanates from the lighted with the focused illumination beam 102 sample 1 15, passes back into the lens 1 12 and then falls on the dichroic beam splitter mirror 1 10. The dichroic beam splitter mirror 1 10 is designed so that it with the light Wavelength of the illumination or excitation beam 102, however, reflects light with the wavelength of the detection or fluorescence beam 1 14th Thus, the detection beam 1 14 at the location of the dichroic beam splitter mirror 1 10 is coupled out of the beam path of the illumination beam 102. Again, the detection beam 1 14 is shown in Figure 4 for the two tilted positions of the scanning mirror 104 with a solid line and a dashed line.

After reflection at the dichroic beam splitter mirror 1 10, the detection beam 1 14 passes through two lenses 1 16, 1 18 and then falls on a dispersive element 120, which is arranged upstream of an image sensor 122. The image sensor 122 has a plurality of

Sensor elements 124 which are individually readable by a controller 126.

The dispersive element 120 is arranged in an intermediate image plane 128, which is optically equivalent to a plane 130 in which the scanning mirror 104 is located. The

Intermediate image plane 128 is also optically conjugate to one in FIG. 4 with 132

designated object plane in which the sample is 1 15. In Figure 4 intermediate image planes 134, 136 and 138 are also shown. The intermediate image plane 134 is a

Plane that is optically equivalent to plane 130 and optically conjugate to object plane 132. The intermediate image plane 136, like the intermediate image plane 138, is optically equivalent to the object plane 132 and optically conjugate to the plane 130.

Since the intermediate image plane 128, in which the dispersive element 120 is located, is optically equivalent to the plane 130, in which the scanning mirror 104 is arranged, the detection beam 1 14 varies with tilting of the scanning mirror 104 only in its

Incident angle, but not in its incident position at the location of the dispersive element 120. The spatial variation of the detection beam 1 14 at the location of the dispersive element 120 corresponds to the extent of the spatial variation of the illumination beam 102 at the location of the scanning mirror 104. The detection beam 1 14 is thus at the location of the dispersive element 120 stationary.

The dispersive element 120 has a predetermined dispersion effect, which results in the detection beam 1 14 being split into its different spectral components. The spectral components are in the representation of Figure 4 in the form of partial beams 1 14-1 bis 1 14-7 illustrates. Again, the partial beams 1 14-1 to 1 14-7 for the two tilt positions of the scanning mirror 104 shown in FIG. 4 are shown once with solid lines and once with dashed lines.

As can be seen in the illustration of Figure 4, the sub-beams 1 14-1 to 1 14-7 quasi form a spectral fan in which the spectral information in a

Angle information is encoded. This angle information is given by the angles at which the various sub-beams 1 14-1 to 1 14-7 emerge from the dispersive element 120 and then strike the individual sensor elements 124 of the image sensor 122.

In the embodiment according to FIG. 4, the illumination beam 102 is intended to scan the sample 15 in two mutually perpendicular scanning directions. The sampling is done in one

Direction faster than in the other direction. The two scanning directions are translated in two respective directions on the image sensor 122. These respective directions are hereinafter also referred to as scanning directions for the sake of simplicity.

In the exemplary embodiment according to FIG. 4, the dispersive element 120 is designed so that the plane in which the detection beam 14 is spectrally split by the dispersive element 120 lies parallel to the slow scanning direction. In this case, the plane of the spectral splitting in the representation according to FIG. 4 is given by the plane of the drawing. Thus, the spectral fan formed by the dispersive element 120 formed of the sub-beams 1 14-1 to 1 14-7 moves in the drawing plane when the scanning mirror 14 is moved in the slow scanning direction. At the same time he tilts through the

Partial beams 1 14-1 to 1 14-7 formed spectral fan in the fast scanning direction perpendicular to the plane of Figure 4, when the scanning mirror in the fast

Scanning direction is moved.

In order to enable a spectrally resolved detection of the detection beam 1 14, the controller 126 detects the present tilting of the scanning mirror 104 and determines therefrom, taking into account the predetermined dispersive effect of the dispersive element 120 those sensor elements 124, just a spectral portion of the detection beam to be considered. 1 14 in the form of one of the partial beams 1 14-1 to 1 14-7 received. These sensor elements 124 then read out the controller 126 at the respective time, at which time the spectral component of the

Detecting beam to detect 1 14. FIG. 5 shows, in a purely schematic representation, a detection optics 140 which is arranged between the dispersive element 120 and the image sensor 122. The

Embodiment of Figure 4 can be supplemented by the detection optics 140.

In a first embodiment, the detection optics 140 is formed solely from a converging lens 142, which has a focal plane 144. The converging lens 142 focuses the partial beams 1 14-1 to 1 14-7 corresponding to the spectral portions of the detection beam 1 14 onto the image sensor 122 so that they fall perpendicularly onto the image sensor 122. In the example according to FIG. 5, the detection beam 1 14 split into the partial beams 1 14-1 to 1 14-7 in the x-z plane moves in the x-direction when the illumination beam 102 scans the sample 15 in the slow scanning direction. On the other hand, it moves on the image sensor 122 in the y direction when the illumination beam 102 scans the sample 15 in the fast scanning direction. In this embodiment, the image sensor 122 is preferably formed as a surface sensor due to the above-described movements of the detection beam 1 14, in which the individual sensor elements 124 are arranged like a matrix in rows (x-direction) and columns (y-direction). Since the sensor elements 124 arranged in a certain column (y-direction) each receive the same spectral component, the signals read out from the sensor elements 124 of this column can be integrated in the spectral detection.

Instead of a surface sensor, a line sensor may also be used as the image sensor 122. In this case, the detection optics 140 is configured to focus the sub-beams 1 14-1 to 1 14-7 on a single line. This can be realized, for example, with an arrangement of three cylindrical lenses. Also for the embodiment is in

Referring to Figure 5 below. In this case, the lens 142 is designed as a cylindrical lens which has an effect on the detection beam 1 14 passing through it only in the x-z plane. In addition, two further cylindrical lenses 144 and 146 are provided, of which the lens 144 is upstream and the lens 146

downstream of the central cylindrical lens 142. The cylindrical lenses 144 and 146 are arranged with their cylinder axes perpendicular to the central cylindrical lens 142.

Accordingly, the cylindrical lenses 144 and 146 influence the passing through them detection beam 1 14 refractive effect only in the yz plane, as the representation of Figure 6 illustrates that shows a yz-section through the detection optics 140. In FIGS. 5 and 6, the lenses shown in dashed lines thus act only on the axis oriented perpendicular to the plane of the drawing. By a suitable choice of the lens spacings can be achieved so that the detection beam 1 14, which passes through this crossed arrangement of the cylindrical lenses 142, 144, 146, in the y direction only in its angle of incidence, not but varies in its incidence position. This allows the use of a line sensor, ie a single-line detector, which detects the total amount of light at all times.

Claims

claims

Scanning microscope with

a lens (1 12), which focuses an illumination beam (102) on a sample (1 15),

a raster element (104) which is arranged upstream of the objective (1 12) and which is adjustable for time-variable deflection of the illumination beam (102) in order to guide the focused illumination beam (102) in a raster motion over the sample (1 15), and

an image sensor (122) onto which the objective (1 12) images a detection beam (1 14) originating from the specimen (1 15) illuminated by the focused illumination beam (102),

wherein the image sensor (122) has a plurality of sensor elements (124) individually readable by a controller (126), via which the detection beam (1 14) is guided in a movement corresponding to the raster movement of the focused illumination beam (102),

characterized by a dispersive element (120) of predetermined dispersion effect upstream of the image sensor (122) which spatially separates different spectral components of the detection beam (1 14) on the image sensor (122), the control (126) for spectrally resolved detection of the detection beam (12). 1 14) detects the temporally variable adjustment of the raster element (104), as a function of this adjustment the sensor elements (124) of the image sensor (122) the spatially separated spectral components of the detection beam (1 14) taking into account the predetermined dispersion effect of the dispersive element (120 ) and read out the sensor elements (124) assigned to the respective spectral components.

Scanning microscope according to claim 1, characterized in that the dispersive element (120) in a plane (128) is arranged, which is optically conjugate to a plane (132) in which the sample (1 15) is arranged.

Scanning microscope according to claim 2, characterized in that the plane (128) in which the dispersive element (120) is arranged, is optically equivalent to a plane (130) in which the grid element (104) is arranged. Scanning microscope according to one of the preceding claims, characterized

characterized in that the raster element (104) guides the illumination beam (102) in a first scanning direction over the sample (15).

Scanning microscope according to claim 4, characterized in that the

Grid element (104) additionally guides the illumination beam (102) across the sample (15) in a second scanning direction perpendicular to the first scanning direction, the movement of the illumination beam (102) being faster in the first scanning direction than in the second scanning direction.

Scanning microscope according to claim 4 or 5, characterized in that the dispersing effect of the dispersive element (120) is predetermined so that the spectral components of the detection beam (1 14) on the image sensor (122) are spatially separated in a direction perpendicular to a direction in which the detection beam (1 14) is passed over the image sensor (122) when the illumination beam (102) in the first scanning direction over the sample (1 15) is guided.

Scanning microscope according to one of the preceding claims, characterized by a between the dispersive element (120) and the image sensor (122)

arranged detection optics (140), the by the dispersive element (120) spectrally split detection beam (1 14) at each adjustment of the

Grid element (104) in its entirety on the image sensor (122) bundles.

Scanning microscope according to claim 7, characterized in that the

Detection optics is a lens in the focal plane, the dispersive element (120) is arranged.

Scanning microscope according to claim 7 or 8, characterized in that the detection optics (140) is formed, the spectrally split detection beam (1 14) at each adjustment of the raster element (104) along a predetermined line on the image sensor (122) to focus.

Scanning microscope according to claim 9, characterized in that the

Detection optics (140) comprises a crossed array of three cylindrical lenses (142, 144, 146), the middle cylinder lens (142) of which has a refractive cut lying in a first plane, while the refractive cuts of the other two cylindrical lenses (144, 146) lie in a plane perpendicular to the first level second level.

1 1. Scanning microscope according to one of the preceding claims, characterized

characterized in that the controller (126) selects at least one of the spectral components and reads out only those sensor elements (124) which have this

are assigned selected spectral component.

12. Scanning microscope according to one of the preceding claims, characterized

characterized in that the image sensor (122) is an area sensor or a line sensor.

13. Scanning microscope according to one of the preceding claims, characterized

characterized in that the dispersive element (120) is a prism or a grating. 14. Scanning microscope according to any preceding claim, characterized in that it is designed for the spectrally resolved detection of the detection beam (1 14) in the non-descanned method.

15. A method for scanning microscopic imaging of a sample (1 14), in which

an illumination beam (102) is focused onto the sample (1 14) by means of an objective (1 12),

a lens element (1 12) upstream raster element (104) to the time

variable deflection of the illumination beam (102) is adjusted to guide the focused illumination beam (102) in a raster motion over the sample (1 14), and

by means of the objective (1 12) a detection beam (1 14), of the with the

Focused illumination beam (102) illuminated sample (1 14) goes out, is focused on image sensor (122),

characterized in that different spectral components of the detection beam (1 14) are spatially separated from one another on the image sensor (122) by means of a predetermined dispersion effect predetermined by the image sensor (122) of a dispersive element (120),

wherein for the spectrally resolved detection of the detection beam (1 14) by means of the controller (126) the time-varying adjustment of the raster element (104) is detected, depending on this adjustment the sensor elements (124) of the Image sensor (122) the spatially separated spectral components of the detection beam (1 14) taking into account the predetermined

Dispersion effect of the dispersive element (120) are assigned and the respective spectral components associated sensor elements (124) are read out.